Let
be a vector space.
is called a Lie algebra if it is equipped with the bilinear operator
, denoted by
, subject to the properties: for every
- (i) [x, x] = 0
- (ii) [x, [y, z]] + [y, [z, x]] + [z, [x, y]] = 0
(ii) is called the Jacobi identity.
Example: For
, define
, the cross product of
and
. The known properties of the cross products show that
is a Lie algebra.
Example: Let
. A member of
is called a derivation. Define
. Then
.
Theorem Let
be a finite-dimensional vector space.
- (i) If
is a Lie algebra consisting of nilpotent elements, then there exists
such that
for every
.
- (ii) If
is solvable, then there exists a common eigenvalue
.
Theorem (Engel)
is nilpotent if and only if
is nilpotent for every
.
Proof: The direct part is clear. For the converse, note that from the preceding theorem that
is a subalgebra of
. Thus,
is nilpotent and so is
.
Theorem
is solvable if and only if
is nilpotent.
Proof: Suppose
is solvable. Then
is a subalgebra of
. Thus,
. Hence,
is nilpotent, and so
is nilpotent. For the converse, note the exact sequence:
![{\displaystyle 0\longrightarrow [{\mathfrak {g}},{\mathfrak {g}}]\longrightarrow {\mathfrak {g}}\longrightarrow {\mathfrak {g}}/{[{\mathfrak {g}},{\mathfrak {g}}]}\longrightarrow 0}](https://wikimedia.org/api/rest_v1/media/math/render/svg/6a96df3ec916ead33753d4c7bf5fae8302d2fdad)
Since both
and
are solvable,
is solvable.
3 Therorem (Weyl's theorem) Every representation of a finite-dimensional semisimple Lie algebra:

is completely reducible.
Proof: It suffices to prove that every
-submodule has a
-submodule complement. Furthermore, the proof reduces to the case when
is simple (as a module) and has codimension one. Indeed, given a
-submodule
, let
be the subspace consisting of elements
such that
is a scalar multiplication. Since any commutator of elements
is zero (that is, multiplication by zero), it is clear that
has dimension 1.
may not be simple, but by induction on the dimension of
, we can assume that. Hence,
has complement of dimension 1, which is spanned by, say,
. It follows that
is the direct sum of
and the kernel of
. Now, to complete the proof, let
be a simple
-submodule of codimension 1. Let
be a Casimir element of
. It follows that
is the direct sum of
and the kernel of
.
(TODO: obviously, the proof is very sketchy; we need more details.)